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Ξ(1690) as...

Ξ(1690) as a K-Σ molecular state

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Ξ(1690) as a K-Σ molecular state

Call No. (NDL)
Z2-868
Bibliographic ID of National Diet Library
11286262
Persistent ID (NDL)
info:ndljp/pid/11286262
Material type
記事
Author
Takayasu Sekihara
Publisher
Oxford University Press
Publication date
2015-09-26
Material Format
Paper・Digital
Journal name
Progress of Theoretical and Experimental Physics : PTEP 2015(9)
Publication Page
-
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コレクション : 国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > その他(Provided by: CiNii Research)

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Digital

Material Type
記事
Author/Editor
Takayasu Sekihara
Publication, Distribution, etc.
Publication Date
2015-09-26
Publication Date (W3CDTF)
2015-09-26
Periodical title
Progress of Theoretical and Experimental Physics : PTEP
No. or year of volume/issue
2015(9)
Volume
2015(9)
ISSN (Periodical Title)
2050-3911
Text Language Code
eng
Persistent ID (NDL)
info:ndljp/pid/11286262
Collection (Materials For Handicapped People:1)
Collection (particular)
国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > その他
Acquisition Basis
オンライン資料収集制度
Date Accepted (W3CDTF)
2019-05-23T16:31:00+09:00
Date Captured (W3CDTF)
2019-01-08
Format (IMT)
application/pdf
Access Restrictions
国立国会図書館内限定公開
Service for the Digitized Contents Transmission Service
図書館・個人送信対象外
Availability of remote photoduplication service
Periodical Title (Persistent ID (NDL))
info:ndljp/pid/11286260
Data Provider (Database)
国立国会図書館 : 国立国会図書館デジタルコレクション

Digital

Summary, etc.
コレクション : 国立国会図書館デジタルコレクション > 電子書籍・電子雑誌 > その他
Access Restrictions
インターネット公開
Has Version
$��(1690)$ as a $\bar{K} ��$ molecular state
Is Referenced By
Theoretical study of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mo>(</mml:mo><mml:mn>1620</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mo>(</mml:mo><mml:mn>1690</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> resonances in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mi>c</mml:mi></mml:msub><mml:mo>→</mml:mo><mml:msup><mml:mi>π</mml:mi><mml:mo>+</mml:mo></mml:msup><mml:mi mathvariant="italic">MB</mml:mi></mml:mrow></mml:math> decays
Analysis of the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mo>(</mml:mo><mml:mn>1620</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math> resonance and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mover accent="true"><mml:mi>K</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mi mathvariant="normal">Λ</mml:mi></mml:mrow></mml:math> scattering length with a chiral unitary approach
Constraining the low-energy <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>S</mml:mi><mml:mo>=</mml:mo><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:math> meson-baryon interaction with two-particle correlations
Why <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1690</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>2120</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:mrow></mml:math> are so narrow
Strong decays of multistrangeness baryon resonances in the quark model
Compositeness of baryonic resonances: Application to the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi mathvariant="normal">Δ</mml:mi><mml:mo>(</mml:mo><mml:mn>1232</mml:mn><mml:mo>)</mml:mo></mml:mrow><mml:mo>,</mml:mo><mml:mspace width="0.16em"/><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mn>1535</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math>, and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>N</mml:mi><mml:mo>(</mml:mo><mml:mn>1650</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:math>resonances
Dynamically generated Ξ(1690)
References
The nature of the lambda(1405) resonance in chiral dynamics
Hadron mass scaling near the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>s</mml:mi></mml:math>-wave threshold
Comprehensive analysis of the wave function of a hadronic resonance and its compositeness
STRUCTURE AND COMPOSITENESS OF HADRON RESONANCES
Measurement of the spin of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ξ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1530</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math>resonance
Remarks on pole trajectories for resonances
Review of Particle Physics
Internal structure of the resonant<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>Λ</mml:mi></mml:mrow></mml:math>(1405) state in chiral dynamics
Couplings in coupled channels versus wave functions: Application to the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>X</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>3872</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math>resonance
Chiral dynamics and the low-energy kaon-nucleon interaction
Observation of Two Charged Bottomoniumlike Resonances in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Υ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>5</mml:mn><mml:mi>S</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math>Decays
Compositeness of dynamically generated states in a chiral unitary approach
Strangeness<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>−</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mo>−</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:math>baryons in a constituent quark model
Quark mass dependence of s-wave baryon resonances
Chiral dynamics in the presence of bound states: kaon–nucleon interactions revisited
Odd-parity light baryon resonances
Coupled-channel analysis of the πη and KK̄ systems near KK̄ threshold
Magnetic moments of the low-lying $$\tfrac{1} {2}^ -$$ octet baryon resonances
Chiral dynamics of the two Λ(1405) states
Study of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si1.gif" overflow="scroll"><mml:msubsup><mml:mi mathvariant="normal">Λ</mml:mi><mml:mi>c</mml:mi><mml:mo>+</mml:mo></mml:msubsup></mml:math> Cabibbo favored decays containing a Λ baryon in the final state
An enhancement at the Σ threshold (1680) MeV observed in K− p reactions at 4.2 GeV/c
Relativistic chiral SU(3) symmetry, large-Nc sum rules and meson–baryon scattering
Observation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>J</mml:mi><mml:mo stretchy="false">/</mml:mo><mml:mi>ψ</mml:mi><mml:mi>p</mml:mi></mml:mrow></mml:math>Resonances Consistent with Pentaquark States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msubsup><mml:mrow><mml:mi mathvariant="normal">Λ</mml:mi></mml:mrow><mml:mrow><mml:mi>b</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msubsup><mml:mo stretchy="false">→</mml:mo><mml:mi>J</mml:mi><mml:mo stretchy="false">/</mml:mo><mml:mi>ψ</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi>p</mml:mi></mml:mrow></mml:math>Decays
Couplings in coupled channels versus wave functions in the case of resonances: Application to the two<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Λ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1405</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math>states
Ξ * resonances inΞ −be interactions
Observation of Cabibbo-suppressed and W-exchange Λ + baryon decays
Strangeness—2 and—3 baryons in a quark model with chromodynamics
Measurements of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>ψ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>3686</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">→</mml:mo><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi mathvariant="normal">Λ</mml:mi><mml:msup><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi></mml:mrow><mml:mrow><mml:mo accent="true" stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:mo>+</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>ψ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>3686</mml:mn><mml:mo stretchy="false">)</mml:mo><mml:mo stretchy="false">→</mml:mo><mml:mi>γ</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mi mathvariant="normal">Λ</mml:mi><mml:msup><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi mathvariant="normal">Ξ</mml:mi></mml:mrow><mml:mrow><mml:mo accent="true" stretchy="false">¯</mml:mo></mml:mrow></mml:mover></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup><mml:mo>+</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mo>.</mml:mo><mml:mi mathvariant="normal">c</mml:mi><mml:mo>.</mml:mo></mml:mrow></mml:math>
Baryons in a relativized quark model with chromodynamics
The spectrum of the nucleons and the strange hyperons and chiral dynamics
Production of hyperons and hyperon resonances in? ? N interactions at 102 and 135 GeV/c*
Effective<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mover accent="true"><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>¯</mml:mo></mml:mrow></mml:mover><mml:mi>N</mml:mi></mml:mrow></mml:math>interaction based on chiral SU(3) dynamics
Origin of resonances in the chiral unitary approach
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ξ</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ω</mml:mi></mml:math>baryons in the Skyrme model
Non-perturbative chiral approach to S-wave interactions
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ξ</mml:mi></mml:math>baryon strong decays in a chiral quark model
Spin, Parity, and Nature of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ξ</mml:mi><mml:mo stretchy="false">(</mml:mo><mml:mn>1620</mml:mn><mml:mo stretchy="false">)</mml:mo></mml:math>Resonance
First observation of the
Data Provider (Database)
国立情報学研究所 : CiNii Research
Bibliographic ID (NDL)
11286262